Jump to
S1C2
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -5226.881284 |
| Energy at 298.15K | -5226.891438 |
| HF Energy | -5226.881284 |
| Nuclear repulsion energy | 416.451708 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3PW91/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Ag |
3114 |
2999 |
0.00 |
|
|
|
| 2 |
Ag |
1483 |
1429 |
0.00 |
|
|
|
| 3 |
Ag |
1289 |
1241 |
0.00 |
|
|
|
| 4 |
Ag |
1075 |
1035 |
0.00 |
|
|
|
| 5 |
Ag |
668 |
644 |
0.00 |
|
|
|
| 6 |
Ag |
189 |
182 |
0.00 |
|
|
|
| 7 |
Au |
3200 |
3082 |
0.74 |
|
|
|
| 8 |
Au |
1110 |
1069 |
4.65 |
|
|
|
| 9 |
Au |
761 |
733 |
6.23 |
|
|
|
| 10 |
Au |
106 |
102 |
4.32 |
|
|
|
| 11 |
Bg |
3177 |
3060 |
0.00 |
|
|
|
| 12 |
Bg |
1288 |
1240 |
0.00 |
|
|
|
| 13 |
Bg |
949 |
914 |
0.00 |
|
|
|
| 14 |
Bu |
3122 |
3007 |
6.73 |
|
|
|
| 15 |
Bu |
1476 |
1422 |
8.52 |
|
|
|
| 16 |
Bu |
1216 |
1171 |
56.95 |
|
|
|
| 17 |
Bu |
595 |
573 |
74.70 |
|
|
|
| 18 |
Bu |
178 |
172 |
7.65 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 12498.7 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 12037.5 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/6-311G**
Point Group is C2h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.492 |
0.570 |
0.000 |
| C2 |
-0.492 |
-0.570 |
0.000 |
| Br3 |
-0.492 |
2.270 |
0.000 |
| Br4 |
0.492 |
-2.270 |
0.000 |
| H5 |
1.114 |
0.578 |
0.892 |
| H6 |
1.114 |
0.578 |
-0.892 |
| H7 |
-1.114 |
-0.578 |
0.892 |
| H8 |
-1.114 |
-0.578 |
-0.892 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5061 | 1.9642 | 2.8403 | 1.0877 | 1.0877 | 2.1664 | 2.1664 |
C2 | 1.5061 | | 2.8403 | 1.9642 | 2.1664 | 2.1664 | 1.0877 | 1.0877 | Br3 | 1.9642 | 2.8403 | | 4.6456 | 2.4978 | 2.4978 | 3.0486 | 3.0486 | Br4 | 2.8403 | 1.9642 | 4.6456 | | 3.0486 | 3.0486 | 2.4978 | 2.4978 | H5 | 1.0877 | 2.1664 | 2.4978 | 3.0486 | | 1.7842 | 2.5102 | 3.0797 | H6 | 1.0877 | 2.1664 | 2.4978 | 3.0486 | 1.7842 | | 3.0797 | 2.5102 | H7 | 2.1664 | 1.0877 | 3.0486 | 2.4978 | 2.5102 | 3.0797 | | 1.7842 | H8 | 2.1664 | 1.0877 | 3.0486 | 2.4978 | 3.0797 | 2.5102 | 1.7842 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
109.152 |
|
C1 |
C2 |
H7 |
112.278 |
| C1 |
C2 |
H8 |
112.278 |
|
C2 |
C1 |
Br3 |
109.152 |
| C2 |
C1 |
H5 |
112.278 |
|
C2 |
C1 |
H6 |
112.278 |
| Br3 |
C1 |
H5 |
106.284 |
|
Br3 |
C1 |
H6 |
106.284 |
| Br4 |
C2 |
H7 |
106.284 |
|
Br4 |
C2 |
H8 |
106.284 |
| H5 |
C1 |
H6 |
110.203 |
|
H7 |
C2 |
H8 |
110.203 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.338 |
|
|
|
| 2 |
C |
-0.338 |
|
|
|
| 3 |
Br |
-0.061 |
|
|
|
| 4 |
Br |
-0.061 |
|
|
|
| 5 |
H |
0.200 |
|
|
|
| 6 |
H |
0.200 |
|
|
|
| 7 |
H |
0.200 |
|
|
|
| 8 |
H |
0.200 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
0.000 |
0.000 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-48.743 |
1.284 |
0.000 |
| y |
1.284 |
-55.686 |
0.000 |
| z |
0.000 |
0.000 |
-49.428 |
|
| Traceless |
| | x | y | z |
| x |
3.813 |
1.284 |
0.000 |
| y |
1.284 |
-6.600 |
0.000 |
| z |
0.000 |
0.000 |
2.787 |
|
| Polar |
| 3z2-r2 | 5.574 |
| x2-y2 | 6.942 |
| xy | 1.284 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.723 |
-2.105 |
0.000 |
| y |
-2.105 |
12.893 |
0.000 |
| z |
0.000 |
0.000 |
5.453 |
<r2> (average value of r
2) Å
2
| <r2> |
426.003 |
| (<r2>)1/2 |
20.640 |
Jump to
S1C1
Energy calculated at B3PW91/6-311G**
| | hartrees |
| Energy at 0K | -5226.877639 |
| Energy at 298.15K | |
| HF Energy | -5226.877639 |
| Nuclear repulsion energy | 449.491631 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at B3PW91/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3157 |
3040 |
0.02 |
101.94 |
0.75 |
0.86 |
| 2 |
A |
3095 |
2981 |
14.92 |
241.74 |
0.02 |
0.03 |
| 3 |
A |
1460 |
1406 |
1.40 |
4.01 |
0.66 |
0.80 |
| 4 |
A |
1313 |
1264 |
23.25 |
4.49 |
0.60 |
0.75 |
| 5 |
A |
1197 |
1153 |
2.40 |
14.53 |
0.75 |
0.86 |
| 6 |
A |
1043 |
1004 |
0.70 |
2.71 |
0.56 |
0.72 |
| 7 |
A |
910 |
876 |
9.24 |
8.67 |
0.43 |
0.60 |
| 8 |
A |
561 |
540 |
8.36 |
16.52 |
0.08 |
0.14 |
| 9 |
A |
229 |
220 |
1.18 |
1.74 |
0.47 |
0.64 |
| 10 |
A |
78 |
75 |
0.22 |
1.43 |
0.73 |
0.84 |
| 11 |
B |
3170 |
3053 |
1.44 |
29.70 |
0.75 |
0.86 |
| 12 |
B |
3087 |
2973 |
2.34 |
54.33 |
0.75 |
0.86 |
| 13 |
B |
1454 |
1400 |
13.33 |
13.68 |
0.75 |
0.86 |
| 14 |
B |
1281 |
1233 |
68.95 |
2.18 |
0.75 |
0.86 |
| 15 |
B |
1127 |
1086 |
3.13 |
5.38 |
0.75 |
0.86 |
| 16 |
B |
847 |
816 |
22.95 |
1.59 |
0.75 |
0.86 |
| 17 |
B |
594 |
572 |
16.63 |
10.57 |
0.75 |
0.86 |
| 18 |
B |
356 |
343 |
6.76 |
2.64 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 12478.6 cm
-1
Scaled (by 0.9631) Zero Point Vibrational Energy (zpe) 12018.1 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at B3PW91/6-311G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.309 |
0.687 |
1.177 |
| C2 |
-0.309 |
-0.687 |
1.177 |
| Br3 |
-0.309 |
1.816 |
-0.293 |
| Br4 |
0.309 |
-1.816 |
-0.293 |
| H5 |
0.024 |
1.213 |
2.090 |
| H6 |
1.394 |
0.649 |
1.101 |
| H7 |
-0.024 |
-1.213 |
2.090 |
| H8 |
-1.394 |
-0.649 |
1.101 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
Br3 |
Br4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.5067 | 1.9534 | 2.9030 | 1.0913 | 1.0884 | 2.1340 | 2.1654 |
C2 | 1.5067 | | 2.9030 | 1.9534 | 2.1340 | 2.1654 | 1.0913 | 1.0884 | Br3 | 1.9534 | 2.9030 | | 3.6843 | 2.4807 | 2.4907 | 3.8644 | 3.0330 | Br4 | 2.9030 | 1.9534 | 3.6843 | | 3.8644 | 3.0330 | 2.4807 | 2.4907 | H5 | 1.0913 | 2.1340 | 2.4807 | 3.8644 | | 1.7809 | 2.4257 | 2.5403 | H6 | 1.0884 | 2.1654 | 2.4907 | 3.0330 | 1.7809 | | 2.5403 | 3.0748 | H7 | 2.1340 | 1.0913 | 3.8644 | 2.4807 | 2.4257 | 2.5403 | | 1.7809 | H8 | 2.1654 | 1.0884 | 3.0330 | 2.4907 | 2.5403 | 3.0748 | 1.7809 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
Br4 |
113.441 |
|
C1 |
C2 |
H7 |
109.408 |
| C1 |
C2 |
H8 |
112.109 |
|
C2 |
C1 |
Br3 |
113.441 |
| C2 |
C1 |
H5 |
109.408 |
|
C2 |
C1 |
H6 |
112.109 |
| Br3 |
C1 |
H5 |
105.607 |
|
Br3 |
C1 |
H6 |
106.437 |
| Br4 |
C2 |
H7 |
105.607 |
|
Br4 |
C2 |
H8 |
106.437 |
| H5 |
C1 |
H6 |
109.579 |
|
H7 |
C2 |
H8 |
109.579 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B3PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.335 |
|
|
|
| 2 |
C |
-0.335 |
|
|
|
| 3 |
Br |
-0.049 |
|
|
|
| 4 |
Br |
-0.049 |
|
|
|
| 5 |
H |
0.185 |
|
|
|
| 6 |
H |
0.198 |
|
|
|
| 7 |
H |
0.185 |
|
|
|
| 8 |
H |
0.198 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.682 |
2.682 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-49.154 |
0.871 |
0.000 |
| y |
0.871 |
-53.705 |
0.000 |
| z |
0.000 |
0.000 |
-44.914 |
|
| Traceless |
| | x | y | z |
| x |
0.156 |
0.871 |
0.000 |
| y |
0.871 |
-6.671 |
0.000 |
| z |
0.000 |
0.000 |
6.515 |
|
| Polar |
| 3z2-r2 | 13.030 |
| x2-y2 | 4.551 |
| xy | 0.871 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.945 |
-0.819 |
0.000 |
| y |
-0.819 |
9.390 |
0.000 |
| z |
0.000 |
0.000 |
8.192 |
<r2> (average value of r
2) Å
2
| <r2> |
316.589 |
| (<r2>)1/2 |
17.793 |